[0001] The present invention relates to epitaxial growth method and apparatus for doping
nitrogen.
[0002] Recently, it has been proposed to increase a recording density in optical recording
and reproduction, magneto-optical recording and reproduction or the like by shortening
the wavelength of laser light used. Therefore, a need has arisen for a short wavelength
laser such as a blue light emitting semiconductor laser or the like. As a blue light
emitting semiconductor laser, a II-VI compound semiconductor of ZnSe system, for example,
formed of II-group element such as zinc, mercury, cadmium, magnesium or the like and
VI-group element such as sulfur, selenium, tellurium or the like has received attention.
[0003] To make a II-VI compound semiconductor have a P-type conductivity, there is known
a method for adding nitrogen (N) thereto as an impurity (e.g., Physics. Review. B
Vol. 27, PP.2419 - 2428 (1983)).
[0004] Further, as a method for adding nitrogen, there is known a method for irradiating
nitrogen molecule or neutral excited species of ammonium molecule (e.g., Japanese
Laid-Open Patent Publication Nos. 63-303899 and 63-303889). Furthermore, as a method
for adding nitrogen, there is known a method for irradiating ion species (see Japanese
Laid-Open Patent Publication No. 63-227027).
[0005] In epitaxial growth apparatus such as an MBE (molecular beam epitaxy) apparatus using
plasma decomposition, a very small flow rate of a plasma generating source is generally
controlled by a variable leak valve. This flow rate is calculated on the basis of
an exhaust speed and a vacuum degree within a vacuum chamber. The vacuum degree within
the vacuum chamber, however, tends to change with deterioration of exhaust ability,
temperature distribution of liquid nitrogen shroud covering the inside of the vacuum
chamber or the like so that the flow rate cannot be reproduced with high accuracy.
Further, since the variable leak valve adjusts the flow rate by a pressing operation,
it is frequently observed that the actual flow rate fluctuates with respect to the
graduation of the supply rate. Therefore, it is very difficult to adjust a very small
flow rate of introduced gas by using such variable leak valve with high accuracy and
high reproducibility.
[0006] The doping amount to the semiconductor is very sensitive to the above flow rate so
that, if the flow rate of introduced gas changes, then it becomes extremely difficult
in the above semiconductor laser to dope a very small amount of nitrogen into the
crystal by plasma decomposition with satisfactory reproducibility.
[0007] Furthermore, in the prior art an RF plasma has been used as a beam source of an excited
species (radical). The electric power applied to an RF plasma generating apparatus
is large and the RF plasma generating apparatus generates much heat. As a result,
when the II-VI compound semiconductor is formed under the vacuum condition of high
vacuum degree, impurity gases such as nitrogen, oxygen, H20 or the like adsorbed to
the inner and outer walls of the RF plasma generating apparatus are separated from
the inner and outer walls and absorbed in the II-VI compound semiconductor as impurities.
There is then the disadvantage that a bad influence is exerted upon an electrical
characteristic of the semiconductor layer.
[0008] Accordingly, it is an object of the present invention to provide an improved epitaxial
growth method and apparatus for doping nitrogen in which the aforesaid shortcomings
and disadvantages encountered with the prior art can be eliminated.
[0009] More specifically, it is an object of the present invention to provide an epitaxial
growth method and apparatus for doping nitrogen in which an amount of gas doped into
a compound semiconductor can be controlled accurately and easily.
[0010] It is another object of the present invention to provide an epitaxial growth method
and apparatus for doping nitrogen in which the occurrence of impurity gas from a plasma
generating apparatus can be suppressed.
[0011] According to a first aspect of the present invention, there is provided an epitaxial
growth system which comprises a vacuum vessel, a plasma generating apparatus for exciting
a doping gas, a source for supplying the doping gas, and a substrate within the vacuum
vessel on which a semiconductor layer is being grown or after having been grown, wherein
the doping gas supply source includes an aperture for doping a part of the doping
gas into the semiconductor layer and an aperture for exhausting a remaining portion
of the doping gas into the vacuum vessel.
[0012] According to a second aspect of the present invention, there is provided an epitaxial
growth method which comprises the steps of growing or having been growing a semiconductor
layer on a substrate within a vacuum vessel by an epitaxy method, doping a part of
gas supplied from a doping gas supply source into the semiconductor layer during or
after the semiconductor layer is grown, and exhausting a remaining gas into the vacuum
vessel, wherein the gas doped into the semiconductor layer is made at least to be
a plasma gas.
[0013] According to a third aspect of the present invention, there is provided an epitaxial
growth method which comprises the steps of depositing a first element selected from
at least one of Hg, Mg, Zn and Cd and a second element selected from at least one
of S, Se and Te on a substrate within a vacuum vessel, and irradiating an excited
species of nitrogen, oxygen molecule or atom excited by an electron-cyclotron-resonance
(ECR) plasma on the substrate.
[0014] The different aspects of the invention as defined above and in the claims may advantageously
be combined together as can the optional features defined in the dependent claims
attached hereto.
[0015] The present invention will be further described in the following detailed description
of illustrative embodiments thereof given by way of example and to be read in conjunction
with the accompanying drawings in which:
FIG. 1 is a diagram showing a structure of an epitaxial growth apparatus according
to an embodiment of the present invention;
FIG. 2 is a cross-sectional view showing a main portion of the epitaxial growth apparatus
according to the embodiment of the present invention;
FIG. 3 is a diagram showing a main portion of the epitaxial growth apparatus according
to another embodiment of the present invention;
FIG. 4 is a diagram showing a molecular beam epitaxy (MBE) apparatus for use in a
manufacturing method of a semiconductor device according to the present invention;
FIG. 5 is a diagram used to explain the manufacturing method according to the present
invention; and
FIGS. 6 and 7 are graphs used to explain the present invention, respectively.
[0016] Embodiments of an epitaxial growth apparatus and a method thereof according to the
present invention will hereinafter be described with reference to the drawings. In
the embodiments of the present invention, nitrogen is doped into a p-type cladding
layer of the ZnSe II-VI compound semiconductor.
[0017] FIG. 1 shows an overall arrangement of an epitaxial growth apparatus according to
the present invention. The inside of a vacuum vessel 2 is exhausted to a predetermined
vacuum degree of, for example, about 10⁻⁹ Torr by an exhausting system (not shown)
as shown by an arrow
a in FIG. 1. A substrate 1 is supported on a substrate holder 16 within the vacuum
vessel 2 and a high frequency (RF) or electron cyclotron resonance (ECR) plasma generating
source 3 is disposed in an opposing relation to the substrate 1. Nitrogen gas from
a high purity nitrogen cylinder or nitrogen purifying apparatus (not shown) is introduced
into the vacuum vessel 2 through a supply rate control unit 5 such as a mass-flow
controller or the like. One portion of the rear stage of the control unit 5 is branched
to exhaust nitrogen gas into the vacuum vessel 2 as shown by an arrow
g in FIG. 1. In FIG. 1, an arrow
m shows an irradiation direction of nitrogen gas molecule. In FIG. 1, reference numerals
17, 18 depict molecular beam apparatus, respectively.
[0018] FIG. 2 shows an example of the plasma generating apparatus 3. In FIG. 2, like parts
corresponding to those of FIG. 1 are marked with the same references and therefore
need not be described in detail. As shown in FIG. 2, from the plasma generating apparatus
3 at its top portion opposing the substrate 1, plasma is generated within a plasma
generating chamber 15 by microwave introduced by a microwave antenna 8. Nitrogen gas
introduced from a gas conduit 11 is separated or excited in the plasm generating chamber
15 and radiated toward the substrate 1 through an aperture 6A formed through a partition
wall 6 of the plasma generating chamber 15 and serving as an irradiation outlet. In
this embodiment, an area of the aperture 6A is 1.0 x 10⁻³ to 1.0 mm². In FIG. 2, reference
numeral 7 depicts a magnet, 10 a sealing member for confining gas, 12 a flange, and
13 a terminal through which microwaves are introduced.
[0019] The plasma generating chamber 15 has a gas exhaust hole 9 bored through its side
wall opposite to the irradiation outlet. In order to protect the substrate 1 from
being directly radiated with nitrogen gas, the nitrogen gas is branched through the
fast exhaust hole 9 and the branched nitrogen gas is exhausted into the vacuum vessel
2 as shown by the arrow
g in FIG. 1.
[0020] In this embodiment, when ZnSe compound semiconductor was grown, the doping of nitrogen
thereinto was carried out under the condition that the supply rate of nitrogen gas
was controlled by the supply rate control unit 5 such as the mass-flow controller
or the like while the nitrogen gas was exhausted. In this case, a substrate temperature
was selected to be 295°C, a beam intensity ratio of Zn and Se was selected to be 1/1.2,
a nitrogen gas flow rate was selected to be 0.2 cm³/minute and plasma of 50W was generated.
When the doping was carried out under the aforementioned conditions, the inside of
the vacuum vessel 2 was reached to a relatively low vacuum degree of about 1 x 10⁻⁵
Torr, i.e., high pressure. According to respective test samples 1 to 3, their p-type
cladding layers having carrier concentration of about 2.5 x 10¹⁷/cm³ could be formed
with satisfactory reproducibility.
[0021] The measured results are illustrated on the table 1 below.
TABLE 1
|
Carrier Concentration(cm⁻³) |
Text Sample 1 |
2.5 x 10¹⁷ |
Text Sample 2 |
2.4 x 10¹⁷ |
Text Sample 3 |
2.6 x 10¹⁷ |
[0022] FIG. 3 shows a structure of a main portion of the epitaxial growth apparatus utilizing
an RF plasma generating apparatus according to another embodiment of the present invention.
In FIG. 3, reference numeral 20 depicts an RF coil, 21 a plasma generating chamber
and 22 a gas conduit. Reference numeral 6 designates a partition wall of the plasma
generating chamber 21 with an aperture 6A as an irradiation outlet similar to the
example shown in FIG. 2. Also in this case, the plasma generating chamber 21 has a
gas exhaust hole 23 bored through the inner wall opposite to the plasma irradiation
outlet. Nitrogen gas is branched through the gas exhaust hole 23 and a part of nitrogen
gas is exhausted into the vacuum vessel 2. Then, the whole flow rate of nitrogen gas
was controlled by the supply rate control unit 5 such as the mass-flow controller
or the like, whereby a carrier concentration could be controlled with satisfactory
reproducibility.
[0023] While the gas exhaust hole is provided on the opposite side to the irradiation outlet
of the plasma generating chamber as described above, the present invention is not
limited thereto and such a variant is also possible. That is, when the gas exhaust
hole was provided through the side wall of the plasma generating chamber and through
the gas conduit within the vacuum vessel 2 or the like, the carrier concentration
could be similarly controlled with satisfactory reproducibiliy without affecting the
crystal growth on the substrate.
[0024] When such gas exhaust hole is formed through the gas conduit provided outside the
vacuum vessel 2, an exhaust system must be connected to the gas exhaust hole. There
is then the risk that a vacuum degree within the vacuum vessel 2 will fluctuate. According
to the present invention, since the gas is exhausted into the vacuum vessel 2, another
exhaust system need not be connected to the gas exhaust hole, i.e., vacuum degree
can be prevented from fluctuating, thereby making it possible to control the flow
rate of the gas with high accuracy.
[0025] While nitrogen gas is doped into the ZnSe system compound semiconductor as described
above, the present invention is not limited thereto and may be applied to the case
that various II-VI compound semiconductors such as ZnTe II-VI semiconductor, Mg II-VI
semiconductor or the like are grown. It is needless to say that the growth apparatus
and the growth method of the present invention are not limited to the aforesaid embodiment
and various changes and modifications could be effected therein.
[0026] As described above, according to the embodiment of the epitaxial growth apparatus
of the present invention, since the nitrogen gas is exhausted into the vacuum vessel
2 via the branched portion that is at the rear stage of the supply rate control unit
5, the whole supply rate of the nitrogen gas can be made relatively large. Therefore,
the flow rate control means of high accuracy such as the mass-flow controller or the
like can be used so that the nitrogen doping amount can be controlled with satisfactory
reproducibility.
[0027] Further, according to the embodiment of the epitaxial growth method of the present
invention, since the nitrogen gas is branched at the rear stage of the supply rate
control unit 5 after the vacuum vessel 2 was exhausted to the predetermined vacuum
degree, the whole flow rate can be made large and the flow rate can be controlled
with satisfactory accuracy, whereby the doping amount of nitrogen gas can be controlled
with satisfactory reproducibility.
[0028] Furthermore, since a part of nitrogen gas is exhausted into the vacuum vessel 2,
a new exhaust system need not be provided, thereby avoiding the vacuum degree within
the vacuum vessel 2 from fluctuating.
[0029] A third embodiment of the present invention will be described below. In the third
embodiment, a p-ZnSe layer formed of ZnSe to which nitrogen (N) is added as impurity
is formed. In this case, selenium (Se) was selected as a first element and zinc (Zn)
was selected as a second element. A nitrogen molecule was utilized as an excited species
and an n-GaAS substrate was utilized as a substrate.
[0030] FIG. 4 schematically shows an arrangement of a molecular beam epitaxy (MBE) apparatus
30 which is suitable for use with a manufacturing method of semiconductor device according
to the present invention. The MBE apparatus 30 is a kind of vacuum evaporating apparatus
and includes a vacuum vessel 31 having an ultra-high vacuum exhausting apparatus (not
shown). The vacuum vessel 31 incorporates therein a plurality of molecular beam sources
(K cells) 32 and a substrate holder 33 for holding a substrate 40.
[0031] One of the most specific features of the MBE apparatus 30 lies in that it includes
an ECR cell 35 which comprises a permanent magnet 36 and a microwave antenna 37. That
is, the plasma generating apparatus includes the ECR cell 35. The permanent magnet
36 can be replaced with an electromagnet. A magnetic force of the magnet can be selected
to b 8.75 x 10⁻²T.
[0032] Nitrogen (N₂) is highly purified by using an adsorption tube (not shown). The nitrogen
is introduced into the ECR cell 35 through a gas conduit 38 made of a stainless steel.
A 2.45 GHz microwave is introduced into the ECR cell 35 by means of the microwave
antenna 37. A plasma gas (excited species of nitrogen molecule) generated within the
ECR cell 35 is exhausted into the vacuum vessel 31 via an aperture 34.
[0033] A manufacturing method of semiconductor device according to the present invention
will be described below.
[0034] Utilizing the apparatus shown in FIG. 4, the n-GaAs substrate 40 whose surface had
been cleaned was mounted on the substrate holder 33. After the vacuum vessel 31 was
exhausted to about 10⁻⁸Pa, according to the conventional method, as shown in FIG.
5, an n-ZnSe first cladding layer 41 was formed on the substrate 40. Further, a (Cd,
Zn) Se active layer 42 was formed on the first cladding layer 42 (see FIG. 5).
[0035] Then, according to the manufacturing method of semiconductor device of the present
invention, as shown in FIG. 5, a p-ZnSe second cladding layer 43 was formed on the
active layer 42. Zinc and selenium of high purity were independently filled into the
respective K cells 32 in advance. Then, the K cells 32 were heated so that they are
adjusted to present proper molecular beam intensities, respectively. The molecular
beam intensity of zinc and selenium was selected to be 1 : 1.2
[0036] A temperature of the substrate 40 was selected to be 300°C. Then, selenium (Se) serving
as the first element and zinc (Zn) serving as the second element were deposited on
the substrate 40. That is, a crystal formed of the first element (Se) and the second
element (Zn) was grown on the active layer 42. At the same time when the crystal was
grown on the active layer 42, the excited species of nitrogen molecule was radiated
on the substrate 40 from the ECR cell 35. Thus, a semiconductor device shown in a
schematic cross-sectional view of FIG. 5 could be manufactured.
[0037] An amount of the radiated excited species (plasma) which is doped into the II-VI
compound semiconductor can be controlled by changing either an electric power applied
to the ECR cell 35 or the opening area of the aperture 34. To change the opening area
of the aperture 34, the vacuum state of vacuum vessel 2 must be broken, returned to
atmospheric pressure and then the aperture must be exchanged. It takes a few weeks
to evacuate the vacuum vessel 21 to high degree after the aperture was exchanged.
Therefore, the amount of nitrogen doped into the II-VI compound semiconductor crystal
must be changed in a wide range by changing an electric power applied to the ECR cell
35.
[0038] As shown in FIG. 6, according to the semiconductor device manufacturing method using
the ECR plasma of the present invention, the amount of nitrogen doped can be controlled
in a wide range and an acceptor representative of p-type conductivity can be introduced
into the II-VI compound semiconductor crystal effectively and accurately. A (A) in
FIG. 6 shows measured results in the case that the opening area of the aperture was
selected to be 8 x 10⁻³ mm² and a (B) in FIG. 6 shows measured results in the case
that the opening area of the aperture was selected to be 7 x 10⁻² mm². In the II-VI
compound semiconductor made of ZnSe, for example, Se and N in the ZnSe crystal is
replaced with N so that, as the amount of N in the ZnSe crystal increases, the amount
of Se decreases. Therefore, it is sufficient that an irradiation density (density
of N element in the II-VI compound semiconductor) at which excited species of nitrogen
molecule is radiated onto the substrate 40 is 10⁻⁶ to 10⁻³ times the deposition density
(density of Se element in the II-VI compound semiconductor) in which Se is deposited
on the substrate 40.
[0039] In addition, as shown in FIG. 6, the electric power applied to the ECR cell 35 is
about half as compared with the electric power (generally 150 to 300W) applied to
the RF plasma generating apparatus. When the electric power applied to the plasma
generating apparatus is increased, a temperature of the plasma generating apparatus
is increased. As a consequence, the plasma generating apparatus generates impurity
gas and this impurity gas is absorbed into the crystal so that the quality of the
compound semiconductor layer is degraded. According to the method using the ECR plasma
of the present invention, the ECR cell 35 serving as the plasma generating apparatus
can be operated with a small electric power, thereby suppressing the occurrence of
impurity gas. Consequently, there can be obtained a semiconductor device of high quality
because photoluminescence of deep level near 600 nm caused by impurities was not observed
as shown in FIG. 7.
[0040] A fourth embodiment of the present invention will be described below. In the fourth
embodiment, nitrogen (N) was added as an impurity and a p-(Mg, Zn) (S, Se) layer was
formed. More specifically, sulfur (S) and selenium (Se) were selected as the first
element and magnesium (Mg) and zinc (Zn) were selected as the second element. Nitrogen
molecule was utilized as the excited species and an n-GaAs substrate was utilized
as the substrate.
[0041] Utilizing the apparatus shown in FIG. 4, the n-GaAs substrate 40 whose surface had
been cleaned was mounted on the substrate holder 33. After the vacuum vessel 31 was
evacuated to about 10⁻⁶Pa, according to the conventional method, an n-(Mg, Zn)(S,
Se) first cladding layer was formed on the substrate 40 and a ZnSe active layer was
formed on the first cladding layer.
[0042] Then, on the basis of the semiconductor device manufacturing method according to
the present invention, a p-(Mg, Zn)(S, Se) second cladding layer was formed on the
active layer. Magnesium, Zinc, sulfur and selenium of high purity serving as raw materials
were respectively filled into the K cells 32 in advance. Then, the K cells 32 were
heated so that they area adjusted to present proper molecular beam intensities, respectively.
In this case, the molecular beam intensity ratio among magnesium, zinc, sulfur and
selenium was selected to be 0.2 : 1 : 0.1 : 1.2.
[0043] A temperature of the substrate 40 was selected to be 300°C and then sulfur (S) and
Selenium (Se) serving as the first element and magnesium (Mg) and Zinc (Zn) serving
as the second element were deposited on the substrate 40, i.e., a crystal made of
the first element (S, Se) and the second element (Mg, Zn) was epitaxially grown on
the active layer. At the same time when the crystal was epitaxially grown on the active
layer, the excited species of nitrogen molecule was radiated onto the substrate 40
from the ECR cell 35. Thus, a II-VI semiconductor device could be manufactured. It
is preferred that the II-VI semiconductor device containing Mg is manufactured by
the method using the ECR plasma according to the present invention because the optical
characteristic and lifetime of the II-VI compound semiconductor containing Mg is easily
affected by impurities as compared with other II-VI compound semiconductors.
[0044] While the preferred embodiments of the present invention have been described so far,
the present invention is not limited thereto and such a variant is also possible.
That is, the GaAs substrate may be replaced with a ZnSe substrate, for example. Further,
the excited species of nitrogen molecule may be replaced with excited species of nitrogen
atom. Furthermore, excited species of oxygen molecule or oxygen atom may be utilized
instead of the excited species of nitrogen molecule. That is, the II-VI compound semiconductor
layer can be given a p-type conductivity by the oxygen.
[0045] Instead of the process that various elements are deposited on the substrate according
to the MBE technique, a gas-source MBE technique, MOMBE technique or technique what
might be called a chemical beam epitaxy might be employed in which a cracking cell
is utilized to impinge raw material gas upon the substrate surface to decompose the
raw material gas on the substrate surface so that elements that are components of
the raw material gas are deposited on the substrate surface.
[0046] The composition of the II-VI compound semiconductor device is not limited to those
of the second and third embodiments and the following variants are also possible by
way of example.
[0047] That is, the substrate is made of n-GaAs, the first cladding layer is made of n-ZnSe,
the active layer is made of Zn(S, Se) and the second cladding layer is made of p-ZnSe
or the substrate is made of p-GaAs, the first cladding layer is made of p-ZnSe, the
active layer is made of (Cd, Zn)Se or Zn(S, Se) and the second cladding layer is made
of n-ZnSe. Further, the substrate is made of p-GaAs, the first cladding layer is made
of p-(Mg, Zn)(S, Se), the active layer is made of ZnSe and the second cladding layer
is made of n-(Mg, Zn)(S, Se). In the aforesaid embodiments, the method of the present
invention is applied to form the p-type compound semiconductor layer.
[0048] Having described preferred embodiments of the invention with reference to the accompanying
drawings, it is to be understood that the invention is not limited to those precise
embodiments and that various changes and modifications could be effected therein by
one skilled in the art without departing from the scope of the invention as defined
in the appended claims.
1. An epitaxial growth apparatus comprising:
a vacuum vessel (2);
a plasma generating apparatus (3) for exciting a doping gas; a source (3, 5) for
supplying said doping gas; and a substrate holder (1) for holding a substrate (16)
within said vacuum vessel (2) and on which a semiconductor layer grown, wherein said
doping gas supply source (3, 5) includes an aperture (6A) for doping said substrate
(1) with a part of said doping gas, characterised in that said doping gas supply source
(3, 5) comprises further aperture (9) for exhausting a remaining portion of said doping
gas into said vacuum vessel (2).
2. Epitaxial growth apparatus according to claim 1, further comprising a means for producing
a vacuum in said vacuum vessel in a range of from 10-3 to 10-6 Torr.
3. Epitaxial growth apparatus according to claim 1 or 2, comprising gas control means
for controlling the amount of gas supplied from said doping gas supply source (5),
to control the amount of doping gas supplied to said plasma generating source (3).
4. Epitaxial growth apparatus according to claim 1, 2 or 3, wherein said vacuum vessel
(2) incorporates therein a material source having II- or VI-group element.
5. Epitaxial growth apparatus according to claim 4, wherein said II-group element is
at least one of Be, Mg, Zn and Cd, and said VI-group element is at least one of S,
Se and Te.
6. Epitaxial growth apparatus according to any one of the preceding claims, wherein said
doping gas is nitrogen.
7. Epitaxial growth apparatus according to any one of the preceding claims, wherein said
semiconductor layer is grown by a molecular beam epitaxy.
8. An epitaxial growth method comprising the steps of: growing a semiconductor layer
on a substrate (1) within a vacuum vessel (2) by an epitaxy method;
doping aid semiconductor layer during or after growth with a part of gas supplied
from a doping gas supply source (3, 5); characterised by:
exhausting a remaining gas into said vacuum vessel (2), wherein said gas doped
into said semiconductor layer is made at least to be a plasma gas.
9. The epitaxial growth method according to claim 8, wherein a vacuum degree within said
vacuum vessel falls in a range of from 10-3 to 10-6 Torr.
10. The epitaxial growth method according to claim 8 or 9, wherein said doping gas is
nitrogen.
11. The epitaxial growth method according to claim 8, 9 or 10 , wherein said semiconductor
grown on said substrate is made of II- and VI-group elements.
12. The epitaxial growth method according to claim 11, wherein said II-group element is
at least one of Hg, Mg, Zn and Cd, and said VI-group element is at least one of S,
Se and Te.
13. An epitaxial growth method comprising the steps of: depositing a first element selected
from at least one of Hg, Mg, Zn and Cd and a second element selected from at least
one of S, Se and Te on a substrate (40) within a vacuum vessel (31) to form a semiconductor
layer; and irradiating an excited species of nitrogen, oxygen molecule or atom excited
by an electron-cyclotron-resonance (ECR) plasma on said semiconductor layer.
14. The epitaxial growth method according to claim 13, wherein a part of said excited
species of nitrogen, oxygen molecule or atom excited by said electron-cyclotron-resonance
(ECR) plasma is radiated on said semiconductor layer and other remaining portion is
exhausted into said vacuum vessel (31).
15. The epitaxial growth method according to claim 13 or 14, wherein at least Mg is selected
as said second element.
16. The epitaxial growth method according to claim 13, 14 or 15, wherein a density at
which said excited species of nitrogen, oxygen molecule or atom is radiated on said
semiconductor layer is 10⁻⁶ to 10⁻³ times the density at which said first element
is deposited on said semiconductor layer.